Abstract

In a recent work [S. Manna, P. Wei, Y. Xie, K. T. Law, P. A. Lee, and J. S. Moodera, Proc. Natl. Acad. Sci. 117, 8775 (2020)], signatures of a pair of Majorana bound states (MBSs) were found in an experimental platform formed by EuS islands deposited on top of a gold surface which was made superconducting through proximity coupling to a superconductor. In this paper, we provide a theoretical understanding for how MBSs can be formed in EuS/Au/superconductor heterostructures. We focus on the strip geometry where a narrow ferromagnetic strip is deposited on a planar structure. We first explicitly map out the topological phase diagram of the EuS/Au/superconductor heterostructure using the lattice Green's function method. Importantly, we find that the chemical potential step between the region with and without EuS covering is a crucial ingredient for the creation of MBS of this setup. Next, we focus on the Bogoliugov quasiparticles that are bound to the region under the EuS by Andreev reflections from the surrounding superconductors. Moreover, we obtain the topological regimes analytically using the scattering matrix method. Notably, we confirm that the normal reflections induced by the chemical potential step are essential for creating finite topological regimes. Furthermore, the area of the topological regimes shows periodic oscillation as a function of chemical potential as well as the sample width. We conclude by showing that the feromagnetic strip geometry holds a number of advantages over other quasi-one-dimensional schemes that have been proposed.

Highlights

  • There has been intense interest in creating Majorana bound states (MBSs) in condensed matter systems

  • We focus on the strip geometry where a ferromagnetic strip is deposited on the (111) surface of gold

  • In this paper we have provided a clear understanding of the topological regimes of the EuS/Au/superconductor heterostructure

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Summary

INTRODUCTION

There has been intense interest in creating Majorana bound states (MBSs) in condensed matter systems. The Zeeman energy is locally enhanced under the ferromagnetic material EuS via the exchange coupling, which enables us to drive the gold surface states under the EuS island into the topological regime with a relatively small in-plane magnetic field. V1, which for simplicity is replaced by its zero frequency limit: Vx ≈ VEuS

Evaluating the Z2 topological invariant
Phase diagram
The importance of the chemical potential step
Topological phase transition boundaries using scattering matrix method
CONCLUSION AND DISCUSSIONS
Proximity gap
Real-space tight-binding Hamiltonian for Majorana wave function
The influence of the choice of the lattice constant a
Vx dependence of the BdG spectrum
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